Difference between revisions of "Nanoscale style machinery at the macroscale"
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'''For main obstacles see page: [[Diffusion slowdown blockade]]''' | '''For main obstacles see page: [[Diffusion slowdown blockade]]''' | ||
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| + | Perhaps also to be covered: Cases where macroscale physics is more limiting compared to nanoscale physics in case of future artificial nanomachinery. | ||
== Related == | == Related == | ||
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* [[Nonthermal self-assembly]] – this works well at the macroscale too | * [[Nonthermal self-assembly]] – this works well at the macroscale too | ||
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| + | * [[Physics change aware scale transposed prototyping]] | ||
| + | * [[Applicability of macro 3D printing for nanomachine prototyping]] | ||
Revision as of 11:29, 9 March 2025
This page is about using the principles of natural nanomachinery (main focus self assembly by movement driven through intense shaking) for assembly at the macroscale.
For main obstacles see page: Diffusion slowdown blockade
Perhaps also to be covered: Cases where macroscale physics is more limiting compared to nanoscale physics in case of future artificial nanomachinery.
Related
- Diffusion slowdown blockade – a potentail hindrance in the incremental path when scaling up selfassembly levels
- Complementary page to: Macroscale style machinery at the nanoscale
This one is not related to many of the common misconceptions about atomically precise manufacturing though.
- Scaling law – selfassembly driven by shaking (even if artificially introduced) scales badly to the macroscale
- Nonthermal self-assembly – this works well at the macroscale too
